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Binary solid-liquid Equilibrium, Melting Point Variation with Composition
Typology: Lecture notes
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Colby College
Gibbs Phase Rule: f = c – p + 2
f = Intensive Degrees of freedom = variance Number of intensive variables that can be changed independently without disturbing the number of phases in equilibrium
p = number of phases gas, homogeneous liquid phases, homogeneous solid phases
c = components Minimum number of independent constituents Case I. No chemical reactions: c = constituents Example 1 : start with methanol and water – 2 components Case II With chemical reactions: Example 2 : start with NaH 2 PO 4 in water -- Ka2 Ka H 2 PO 4 -^ →← HPO 4 2-^ + H+^ →← PO 4 3-^ + H+ Constituents: Na+, H+, H 2 PO 4 - , HPO 4 2-, PO 4 3-, H 2 O but only 2 components -- NaH 2 PO 4 and H 2 O. Example 3 : start with NaH 2 PO 4 and Na 2 HPO 4 in water -- Same constituents: Na+, H+, H 2 PO 4 - , HPO 4 2-, PO 4 3-, H 2 O but now 3 components -- NaH 2 PO 4 , Na 2 HPO 4 , and H 2 O.
Need to know: T, P, y A, y B, x A, x B
total intensive variables = c p + 2
But y A + y B = 1
x A + x B = 1 Get p such equations, one for each phase:
Independent variables = c p + 2 – p
But, chemical potential is everywhere equal: μA( x A) = μA(g) μB( x B) = μB(g) Get p–1 for each component Get c( p–1) such equations: Independent variables = c p + 2 – p – c( p–1)
f = c – p + 2
A & B liquid
μA(g) μA( x A)
μB( x B)
μB(g)
x A + x B =
A & B vapor
y A + y B =
f ' = c – p + 1 P = cst
(^0) x A, y A →^1
liquid A & B f ' = 2
vapor A & B
T (^) f ' = 1
f ' = 2
T (^) bA*
T (^) bB*
Colby College
f ' = c – p + 1 cst. P f "= c – p cst. T&P
Binary solid-liquid Equilibrium Melting Point Variation with Composition c = 2 p = 3
liquid, pure solid A, pure solid B
Solid-liquid 2-phase region: f ' = 2 – 2 + 1 = 1
Eutectic: f ' = 2 – 3 + 1 = 0 invariant at cst P
For NaCl in water: Eutectic -21.1 oC at 23% wt/wt giving NaCl·2H 2 O
Add One Extensive Independent Variable for Each Phase: Gibbs energy is extensive: Degrees of freedom:
D = f + p
Solid-liquid 2-phase region: f " = 2 – 2 = 0 D " = f " + p = 0 + 2 = 2
dG = μA dnA + μB dnB dnA and dnB: totals for both phases
since: μA(s) = μA(l), and μB(s) = μB(l) (doesn’t matter which phase)
A & B liquid
Solid A & Solid B
P = cst
(^0) x A → 1
solid A & solid B
liquid A & B T f ' = liq. & solid B
f ' = liq. & solid A f ' =
f ' =
f ' = c – p + 1